We study the effect of long-range Coulomb interaction on the disordered stats. We will address the metal-insulator transition which takes place due to the Coulomb interaction between electrons in presence of disorder. Our results shows that this transition comes along with the critical behavior of the auto-correlation function of the local density of states(LDoS) around the Fermi energy. A scaling analysis of the LDo correlation demonstrates new multi-fractal structure with a new correlation dimension which is significantly larger than at a non-interacting Anderson transition. At the interaction-driven transition the states at the Fermi level become critical, while the bulk of the spectrum remains ed-localized up to substantially stronger interactions. The mobility edge stays close to the Fermi energy in a wide range of disorder strength, as the interaction strength is further increased. The localization transition is concomitant with the quantum-to- 0cm 0cm 0pt" of metastable Hartree-Fock solutions that suggest the onset of a glassy regime with poor screening properties.